Inspired by the thread/state correspondence, it is natural to construct a novel toy model of the holographic principle, as shown in figure REF (a). We can divide the holographic boundary quantum system into extremely large \(N\)  non-overlapping adjacent subregions (called \(elementary ~regions\) ), denoted as \({A_1}\) , \({A_2}\) , ..., \({A_N}\) , then introduce a \(multiflow\)  composed of \(N\left( {N - 1} \right)/2\)  \(component~ flows\)  to describe a locking thread configuration that can lock all these elementary regions and a set of non-intersecting \(composite~ regions\)  (the unions of elementary regions) simultaneously. In addition, we also require that each component flow flux in the locking bit thread configuration satisfies the so-called “CFF=PEE” scheme [1]}, i.e.,

\({F_{ij}} = \frac{1}{2}\left( {S\left( {\tilde{A} \cup {A_i}} \right) + S\left( {\tilde{A} \cup {A_j}} \right) - S\left( {\tilde{A}} \right) - S\left( {{A_i} \cup \tilde{A} \cup {A_j}} \right)} \right),\) 
